首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   5861篇
  免费   351篇
  国内免费   334篇
化学   349篇
晶体学   30篇
力学   1280篇
综合类   59篇
数学   484篇
物理学   515篇
综合类   3829篇
  2024年   20篇
  2023年   61篇
  2022年   100篇
  2021年   102篇
  2020年   129篇
  2019年   109篇
  2018年   116篇
  2017年   144篇
  2016年   213篇
  2015年   205篇
  2014年   235篇
  2013年   269篇
  2012年   290篇
  2011年   268篇
  2010年   184篇
  2009年   253篇
  2008年   265篇
  2007年   339篇
  2006年   307篇
  2005年   304篇
  2004年   259篇
  2003年   255篇
  2002年   229篇
  2001年   211篇
  2000年   193篇
  1999年   173篇
  1998年   141篇
  1997年   138篇
  1996年   122篇
  1995年   129篇
  1994年   126篇
  1993年   110篇
  1992年   104篇
  1991年   92篇
  1990年   98篇
  1989年   79篇
  1988年   61篇
  1987年   38篇
  1986年   33篇
  1985年   9篇
  1984年   7篇
  1982年   3篇
  1981年   6篇
  1980年   3篇
  1979年   4篇
  1977年   3篇
  1971年   1篇
  1967年   1篇
  1959年   1篇
  1957年   2篇
排序方式: 共有6546条查询结果,搜索用时 15 毫秒
1.
Luca Cimbaro 《哲学杂志》2019,99(12):1499-1514
A unified theory captures both brittle and ductile fracture. The fracture toughness is proportional to the applied stress squared and the length of the crack. For purely brittle solids, this criterion is equivalent to Griffith's theory. In other cases, it provides a theoretical basis for the Irwin-Orowan formula. For purely ductile solids, the theory makes direct contact with the Bilby-Cottrell-Swinden model. The toughness is highest in ductile materials because the shielding dislocations in the plastic zone provide additional resistance to crack growth. This resistance is the force opposing dislocation motion, and the Peach-Koehler force overcomes it. A dislocation-free zone separates the plastic zone from and the tip of the crack. The dislocation-free zone is finite because molecular forces responsible for the cohesion of the surfaces near the crack tip are not negligible. At the point of crack growth, the length of the dislocation-free zone is constant and the shielding dislocations advance in concert. As in Griffith's theory, the crack is in unstable equilibrium. The theory shows that a dimensionless variable controls the elastoplastic behaviour. A relationship for the size of the dislocation-free zone is derived in terms of the macroscopic and microscopic parameters that govern the fracture.  相似文献   
2.
针对裂缝热中子示踪探测方法,从中子双组扩散理论入手结合蒙特卡洛数值模拟方法,分析压裂前后地层热中子分布影响因素,并模拟不同类型示踪剂及含量的热中子裂缝响应规律,筛选最佳示踪剂并给出其在支撑剂中含量的上、下限。结果表明:压裂前后热中子计数变化量主要受裂缝宽度和标记支撑剂中示踪剂含量的影响;钆对裂缝宽度变化反应最灵敏,钆元素是作为标记支撑剂的最佳示踪元素;随支撑剂中Gd 2O 3含量的增加,热中子计数率降低,热中子计数变化量D增加;示踪剂中氧化钆的上、下限值随裂缝宽度呈指数降低,且当裂缝宽度为1.0 cm时,Gd 2O 3的质量分数上限为0.68%,下限为0.03%。  相似文献   
3.
4.
A model is developed for the formation and propagation of cracks in a material sample that is heated at its top surface, pyrolyses, and then thermally degrades to form char. In this work the sample is heated uniformly over its entire top surface by a hypothetical flame (a heat source). The pyrolysis mechanism is described by a one-step overall reaction that is dependent nonlinearly on the temperature (Arrhenius form). Stresses develop in response to the thermal degradation of the material by means of a shrinkage strain caused by local mass loss during pyrolysis. When the principal stress exceeds a prescribed threshold value, the material forms a local crack. Cracks are found to generally originate at the surface in response to heating, but occasionally they form in the bulk, away from ever-changing material boundaries. The resulting cracks evolve and form patterns whose characteristics are described. Quantities examined in detail are: the crack spacing in the pyrolysis zone; the crack length evolution; the formation and nature of crack loops which are defined as individual cracks that have joined to form loops that are disconnected from the remaining material; the formation of enhanced pyrolysis area; and the impact of all of the former quantities on mass flux. It is determined that the mass flux from the sample can be greatly enhanced over its nominal (non-cracking) counterpart. The mass efflux profile qualitatively resembles those observed in Cone Calorimeter tests.  相似文献   
5.
塔东热液地质作用机制及对储层的改造意义   总被引:1,自引:0,他引:1  
塔东地区断裂发育,早期发育的断裂与晚期断裂之间存在相互改造、叠加、复合的过程,深大断裂沟通多套地层,断裂活动期形成的挤压破碎带和断裂裂缝带作为岩浆热液上升通道,为热液溶蚀作用改造储层提供了有利条件,因此,识别出热液期次对塔东白云岩储层成因机制具有重要意义。通过对钻井岩芯、岩屑及岩石薄片、铸体薄片观察鉴定分析,在区内下古生界碳酸盐岩中识别和发现了钠长石化作用和自生羽毛状伊利石沉淀,也是塔里木盆地内的首次发现,并通过对包裹体均一温度,碳氧同位素等地化特征研究,揭示其成岩流体源于岩浆热液,丰富了区内热液作用的矿物学标志,进一步识别出区内存在3期热液作用,通过对3期热液作用的机制及其储渗空间意义的研究,总结出第I期热液作用对于储层形成意义不大,第Ⅱ期热液作用主要发育在局限的沉积环境,第Ⅲ期热液溶蚀形成溶蚀缝孔洞,与天然气运移聚集匹配良好,构成了区内天然气聚集成藏的主要储渗空间。  相似文献   
6.
基于神经网络智能天线的一种波达方向估计方法   总被引:1,自引:0,他引:1  
该文提出利用径向基函数神经网络来估计无线通信中智能天线的信号到达方向.为了减少输入,利用信号相关阵的对称性质,仅考虑相关阵中的上三角或下三角的部分元素作为网络的输入量,计算量较小.计算机模拟结果表明,该方案是有效的.  相似文献   
7.
主要阐述化工新工艺必须以人类的可持续发展为前提,强调资源的综合合理利用,注重环境保护等,并通过实例说明化工新工艺对可持续发展的贡献。  相似文献   
8.
The transport of monodisperse as well as polydisperse colloid suspensions in a two-dimensional, water saturated fracture with spatially variable and anisotropic aperture is investigated with a particle tracking model. Both neutrally buoyant and dense colloid suspensions are considered. Although flow and transport in fractured subsurface formations have been studied extensively by numerous investigators, the transport of dense, polydisperse colloid suspensions in a fracture with spatially variable and anisotropic aperture has not been previously explored. Simulated snapshots and breakthrough curves of ensemble averages of several realizations of a log-normally distributed aperture field show that polydisperse colloids exhibit greater spreading than monodisperse colloids, and dense colloids show greater retardation than neutrally buoyant colloids. Moreover, it is demonstrated that aperture anisotropy oriented along the flow direction substantially increases colloid spreading; whereas, aperture anisotropy oriented transverse to the flow direction retards colloid movement.  相似文献   
9.
A previously developed laser spallation technique has been modified to measure the tensile strength of thin film interfaces in-situ at temperatures up to 1100°C. Tensile strengths of Nb/A-plane sapphire, FeCrAl/A-plane sapphire and FeCrAlY/A-plane sapphire were measured up to 950°C. The measured strengths at high temperatures were substantially lower compared with their corresponding strengths at ambient temperature. For example, at 850°C, the interface tensile strength for the Nb/sapphire (151 ± 17 MPa), FeCrAl/sapphire (62 ± 8 MPa) and FeCrAlY/sapphire (82 ± 11 MPa) interface systems were lower by factors of approximately, 3, 5, and 8, respectively, over their corresponding ambient values. These results underscore the importance of using such in-situ measured values under operating conditions as the failure criterion in any life prediction or reliability models of such coated systems where local interface temperature excursions are expected. The results on alloy film interfaces also demonstrate that the presence of Y increases the strength of FeCrAl/Al2O3 interfaces.  相似文献   
10.
Films of amorphous polystyrene (PS) with a weight-average molecular weight (Mw) of 225 × 103 g/mol were bonded in a T-peel test geometry, and the fracture energy (G) of a PS/PS interface was measured at the ambient temperature as a function of the healing time (th) and healing temperature (Th). G was found to develop with (th)1/2 at Th = Tg-bulk − 33 °C (where Tg-bulk is the glass-transition temperature of the bulk sample), and log G was found to develop with 1/Th at Tg-bulk − 43 °C ≤ ThTg-bulk − 23 °C. The smallest measured value of G = 1.4 J/m2 was at least one order of magnitude larger than the work of adhesion required to reversibly separate the PS surfaces. These three observations indicated that the development of G at the PS/PS interface in the temperature range investigated (<Tg-bulk) was controlled by the diffusion of chain segments feasible above the glass-transition temperature of the interfacial layer, in agreement with our previous findings for fracture stress development at several polymer/polymer interfaces well below Tg-bulk. Close values of G = 8–9 J/m2 were measured for the symmetric interfaces of polydisperse PS [Mw = 225 × 103, weight-average molecular weight/number-average molecular weight (Mw/Mn) = 3] and monodisperse PS (Mw = 200 × 103, Mw/Mn = 1.04) after healing at Th = Tg-bulk − 33 °C for 24 h. This implies that the self-bonding of high-molecular-weight PS at such relatively low temperatures is not governed by polydispersity. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 1861–1867, 2004  相似文献   
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号